Degeneracies of energy levels in the Kitaev quantum double model for arbitrary discrete group G and genus are expressed via S-matrix elements, giving the exact partition function for finite systems.
Title resolution pending
8 Pith papers cite this work. Polarity classification is still indexing.
8
Pith papers citing it
citation-role summary
background 1
citation-polarity summary
verdicts
UNVERDICTED 8roles
background 1polarities
background 1representative citing papers
A thermometry technique using correlations, susceptibility, and high-T expansion applied to a Kagome lattice Rydberg experiment gives T=0.55J and entropy per site 0.67 ln(2), indicating the system is not yet in the quantum spin liquid regime.
A scheme is developed to engineer strong three-body interactions in Rydberg atom lattices, allowing the effective Hamiltonian and emergent quantum phases to be modified compared to two-body-only systems.
Long-range dipolar interactions on a breathed Kagome lattice stabilize a chiral spin liquid, identified via DMRG and proposed for adiabatic preparation and edge-mode detection.
A 256-qubit Rydberg simulator quantitatively reproduces the magnetization curves and antiferromagnetic transition of TmMgGaO4 while revealing thermalization after quenches.
EIT cooling with fluorescence imaging achieves 99.7% readout fidelity and 98.2% survival for 87Rb atom arrays in 2.3 G fields, validated up to 10 G.
Rydberg atoms on a triangular lattice host a deconfined quantum critical point between 1/3 and 2/3 filling phases, with predicted critical exponents, emergent U(1) symmetry in a CFT, and numerical confirmation.
A mapping of the Z3 Rabi model to a qubit-boson ring enables superconducting implementations and a coupled chain for the Z3 Potts model.
citing papers explorer
-
Partition function of the Kitaev quantum double model
Degeneracies of energy levels in the Kitaev quantum double model for arbitrary discrete group G and genus are expressed via S-matrix elements, giving the exact partition function for finite systems.
-
Thermometry for a Kagome Lattice Dipolar Rydberg Simulator
A thermometry technique using correlations, susceptibility, and high-T expansion applied to a Kagome lattice Rydberg experiment gives T=0.55J and entropy per site 0.67 ln(2), indicating the system is not yet in the quantum spin liquid regime.
-
Three-body interactions in Rydberg lattices
A scheme is developed to engineer strong three-body interactions in Rydberg atom lattices, allowing the effective Hamiltonian and emergent quantum phases to be modified compared to two-body-only systems.
-
A Dipolar Chiral Spin Liquid on the Breathed Kagome Lattice
Long-range dipolar interactions on a breathed Kagome lattice stabilize a chiral spin liquid, identified via DMRG and proposed for adiabatic preparation and edge-mode detection.
-
One-to-one quantum simulation of a frustrated magnet with 256 qubits
A 256-qubit Rydberg simulator quantitatively reproduces the magnetization curves and antiferromagnetic transition of TmMgGaO4 while revealing thermalization after quenches.
-
Loading and Imaging Atom Arrays via Electromagnetically Induced Transparency
EIT cooling with fluorescence imaging achieves 99.7% readout fidelity and 98.2% survival for 87Rb atom arrays in 2.3 G fields, validated up to 10 G.
-
Deconfined quantum criticality on a triangular Rydberg array
Rydberg atoms on a triangular lattice host a deconfined quantum critical point between 1/3 and 2/3 filling phases, with predicted critical exponents, emergent U(1) symmetry in a CFT, and numerical confirmation.
-
From coupled $\mathbb{Z}_3$ Rabi models to the $\mathbb{Z}_3$ Potts model
A mapping of the Z3 Rabi model to a qubit-boson ring enables superconducting implementations and a coupled chain for the Z3 Potts model.